Conservation of angular momentum in an inelastic collision?

AI Thread Summary
In the discussion on the conservation of angular momentum during an inelastic collision, a clay blob collides with a bar on a frictionless table, raising questions about final speed and angular velocity. The calculations for the center of mass and moment of inertia are crucial, with the need to apply the Parallel Axis Theorem for accurate results. Participants clarify the contributions of the clay and bar to the system's moment of inertia, emphasizing the importance of calculating the inertia about the new center of mass. The initial confusion about the moment of inertia is resolved, leading to the correct angular speed calculation. The discussion highlights the complexities of angular momentum conservation in inelastic collisions.
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Homework Statement


On a frictionless table, a glob of clay of mass 0.380 kg strikes a bar of mass 0.9 kg perpendicularly at a point 0.550 m from the center of the bar and sticks to it.
a) a) If the bar is 1.300 m long and the clay is moving at 8.100 m/s before striking the bar, what is the final speed of the center of mass? (Got this, 2.405m/s)
b)At what angular speed does the bar/clay system rotate about its center of mass after the impact (in rad/s)?

Homework Equations



Li=Lf
L=r x p =mrv (when theta = 90, as in this case)
L=Iw
I of a rod = (ML2)/12
xcenter of mass=Ʃmx/Ʃm

The Attempt at a Solution


m = mass of clay
M=mass of bar
u=clay's initial speed
r=the distance from the clay to the new CM

So I set one end of the bar as x=0 and the other as x=1.3 to calculate CM
CM=((0.38)(0.65+0.55)+(0.65)(0.9))/(0.9+0.38)=0.81328m from the end of the bar
r=1.2-0.81328=0.3867m

Initial angular velocity=mru
Final " "=((1/12)ML2+mr2
so ω=(mru)/((1/12)(ML2+mr2)
When I plug in my values, I get the wrong answer, it is supposed to be 5.73. Where am I going wrong? I have spent hours at this :( I'm so frustrated!

Homework Statement


Homework Equations


The Attempt at a Solution

 
Last edited:
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mot said:

Homework Statement


On a frictionless table, a glob of clay of mass 0.380 kg strikes a bar of mass 0.9 kg perpendicularly at a point 0.430 m from the center of the bar and sticks to it.
a) a) If the bar is 1.300 m long and the clay is moving at 8.100 m/s before striking the bar, what is the final speed of the center of mass? (Got this, 2.405m/s)
b)At what angular speed does the bar/clay system rotate about its center of mass after the impact (in rad/s)?

Homework Equations



Li=Lf
L=r x p =mrv (when theta = 90, as in this case)
L=Iw
I of a rod = (ML2)/12
xcenter of mass=Ʃmx/Ʃm

The Attempt at a Solution


m = mass of clay
M=mass of bar
u=clay's initial speed
r=the distance from the clay to the new CM

So I set one end of the bar as x=0 and the other as x=1.3 to calculate CM
CM=((0.38)(0.65+0.55)+(0.65)(0.9))/(0.9+0.38)=0.81328m from the end of the bar
r=1.2-0.81328=0.3867m

Where are the data in red come from?

mot said:
Initial angular velocity=mru
Final " "=((1/12)ML2+mr2

You need the moment of inertia with respect to the new CM. (1/12)ML2 is the moment of inertia with respect to the centre of the rod.


ehild
 
Sorry I made a typo in the question, 0.43 should have been 0.55. I've fixed it now. (1.2 is 0.65+0.55, the "position" of the clay on the rod with respect to the end).

That's what I was thinking with the moment of inertia...but doesn't adding the mr^2 take that into account?
I could also do I=Ʃmr^2, where r is the distance from the new CM
=(0.9)(0.81328-0.65)^2+(0.38)(0.3867)^2=0.0808

and my old I=((1/12)(0.9)(1.3^2)+(0.38)(0.3867^2))=0.1836

The new I gives me 14.7rad/s when I plug it into the equation:(
 
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mot said:
That's what I was thinking with the moment of inertia...but doesn't adding the mr^2 take that into account?
No. That's the blob of clay's contribution to the moment of inertia of the bar+clay system. The bar's contribution is the moment of inertia of the bar about the combined center of mass.

Hint: Parallel axis theorem.
 
Thanks so much guys, I got it! It seemed so obvious this morning, I guess that's why you shouldn't do physics at 2am. I was comparing it to a question I had done with a mass on a rotating disc, forgetting that the disc was still rotating about the central axis
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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